1990
DOI: 10.1119/1.16243
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Bell’s theorem without inequalities

Abstract: It is demonstrated that the premisses of the Einstein–Podolsky–Rosen paper are inconsistent when applied to quantum systems consisting of at least three particles. The demonstration reveals that the EPR program contradicts quantum mechanics even for the cases of perfect correlations. By perfect correlations is meant arrangements by which the result of the measurement on one particle can be predicted with certainty given the outcomes of measurements on the other particles of the system. This incompatibility wit… Show more

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Cited by 2,250 publications
(1,767 citation statements)
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“…When three particles are prepared in the quantum state known as the GHZ state, there are three observables X 1 , X 2 and X 3 , each corresponding to one particle, and taking one of two possible values +1 or −1, such that the product of the revealed outcomes must equal −1 (for details see Greenberger et al 1990;Bigaj 2006, pp. 143-145).…”
Section: Bennett's Fork Theorymentioning
confidence: 99%
“…When three particles are prepared in the quantum state known as the GHZ state, there are three observables X 1 , X 2 and X 3 , each corresponding to one particle, and taking one of two possible values +1 or −1, such that the product of the revealed outcomes must equal −1 (for details see Greenberger et al 1990;Bigaj 2006, pp. 143-145).…”
Section: Bennett's Fork Theorymentioning
confidence: 99%
“…As a result, it is the so-called "classical" version of the CHSH inequality-and most if not all of the other guises that Bell's inequalities can take on-that is suspect. (This includes versions that do not directly involve inequalities, such as the GHZ formulation, [26] but which require statistical arguments when experimental justification is sought. This is covered in more detail in a previous paper.…”
Section: E(qs) + E(rs) + E(rt ) − E(qt ) ≤mentioning
confidence: 99%
“…It is composed out of two semi-classical, distinct states, each of which a direct product of two coherent states in, in total, four mutually orthogonal modes, i.e., |χ is a "cat state" [109]. It is an entangled coherent state with nonclassical correlations of the GHZ type [57,[117][118][119]. From an experimental point of view, handling |χ may prove difficult: the state will be very sensitive to decoherence, and its creation requires a special, highly nonlinear MZI that, at the time of this writing, is not readily available.…”
Section: The Simultaneously Both Open and Closed Configurationmentioning
confidence: 99%